the bulge halo conspiracy of elliptical galaxies
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The bulge-halo conspiracy of elliptical galaxies Rhea Remus, - PowerPoint PPT Presentation

USM The bulge-halo conspiracy of elliptical galaxies Rhea Remus, Andreas Burkert, Jens Thomas, Peter Johansson, Thorsten Naab, Ludwig Oser, Klaus Dolag Remus + 2012, submitted Barnes 88; Hernquist 89; Springel+ 02; Naab+ 06; Khochfar+ 06; Cox+


  1. USM The bulge-halo conspiracy of elliptical galaxies Rhea Remus, Andreas Burkert, Jens Thomas, Peter Johansson, Thorsten Naab, Ludwig Oser, Klaus Dolag Remus + 2012, submitted Barnes 88; Hernquist 89; Springel+ 02; Naab+ 06; Khochfar+ 06; Cox+ 06; Lotz+ 08,10; Hopkins+ 08; Johansson+ 09; Jesseit+09; Oser+ 10

  2. Atlas 3D and the stellar structure of ellipticals (Cappellari+11; Emsellem+11; Bois+ 11)

  3. Dark matter in ellipticals: The PN survey (Mendez+ 01; Romanowski+ 03; Dekel+ 05)

  4. SLACS strong lensing survey (Auger+ 10; Barnabe+ 11; Lyskova+ 12) ρ total  r − 2

  5. • Schwarzschild models • 10%-50% dark matter within half light radius

  6. Isolated binary mergers (Johansson+ 09)

  7. Isolated binary mergers (Johansson+ 09) • Controlled initial conditions • Observed formation scenario • Realistic progenitor spirals • No cosmological treatment

  8. Cosmological resimulations (Oser+ 10, 11) • More “realistic” (???) initial conditions • Full mass range of ellipticals • No spirals as progenitors 17 central ellipticals, 4 substructure ellipticals

  9. The halo-spheroid conspiracy ρ tot  r − 2

  10. The halo-spheroid conspiracy in cosmological simulations

  11. Binary mergers • Close to solution of isotropic Jeans equation • Very close to isothermal Cosmo • Very close to isotermal • Large spread in density slope • Steep slopes show large deviation from isotropic Jeans solution

  12. Binary dark matter stars Cosmo

  13. Stellar dispersion slope versus total density slope • Comparison with Thomas et al. favors multiple merger origin • Steepness of density slope depends critically on central concentration of baryonic component ( see however van Dokkum & Conroy 11,12: Conroy & van Dokkum 12)

  14. Slope evolution and violent relaxation

  15. Slope evolution and violent relaxation

  16. Slope evolution and violent relaxation Massive elliptical: Low-mass elliptical: multiple substantial mergers minor mergers and accretion

  17. Summary • The stellar and dark matter density and velocity dispersion profiles of ellipticals are not power laws. • Their combined profiles can however be well fitted by power-laws in the radius range of 0.1 to 3 reff. • Mergers of 2-component systems lead to combined power-law profiles that are isothermal (violent relaxation???). • Deviations from isothermal profiles therefore contain valuable information about the accretion history of a given galaxy. • Cosmological simulations, despite their known caveats, are in good agreement with recent observations of Coma ellipticals.

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